Explain the refraction of a plane wavefront with a thin convex mirror.
Figure shows the plane wavefront $\mathrm{XY}$ of a parallel beam of light incident to a thin convex lens and rays coming out through the thin convex lens is shown to be concentrated at second focus point. To draw a wavefront corresponding to these rays, the circles should be drawn by accepting second focus as a centre. The arc $X^{\prime} Y^{\prime}$ of such circles is shown in the figure.
This arc is the wavefront corresponding to the refracted rays at some instant.
Here the distances from $A$ to $a$ and $C$ to $c$ are greater then B to $b$. So the light has taken more distance in the lens going for $B$ to $b$ and the velocity of light in the material of lens is less. Hence, the point $b$ on the wavefront lags behind $a$ and $c$.
What is the shape of the wavefront in each of the following cases:
$(a)$ Light diverging from a point source.
$(b)$ Light emerging out of a convex lens when a point source is placed at its focus.
$(c)$ The portion of the wavefront of light from a distant star intercepted by the Earth.
Consider a point at the focal point of a convergent lens. Another convergent lens of short focal length is placed on the other side. What is the nature of the wavefronts emerging from the final image ?
Explain how to get a new wavefront in time $\pi $ using Huygen's principle for plane wavefront.
What is the most important point of Huygen's wave theory ?
Ray diverging from a point source from a wave front that is